Learning objectives
Learning Objectives
By the end of this section, you will be able to:
- List the three properties of a conductor in electrostatic equilibrium.
- Explain the effect of an electric field on free charges in a conductor.
- Explain why no electric field may exist inside a conductor.
- Describe the electric field surrounding Earth.
- Explain what happens to an electric field applied to an irregular conductor.
- Describe how a lightning rod works.
- Explain how a metal car may protect passengers inside from the dangerous electric fields caused by a downed line touching the car.
Conductors contain free charges that move easily. When excess charge is placed on a conductor or the conductor is put into a static electric field, charges in the conductor quickly respond to reach a steady state called electrostatic equilibrium.
import-auto-id3230544 shows the effect of an electric field on free charges in a conductor. The free charges move until the field is perpendicular to the conductor’s surface. There can be no component of the field parallel to the surface in electrostatic equilibrium, since, if there were, it would produce further movement of charge. A positive free charge is shown, but free charges can be either positive or negative and are, in fact, negative in metals. The motion of a positive charge is equivalent to the motion of a negative charge in the opposite direction.
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Original figure description: In part a, an electric field E exists at some angle with the horizontal applied on a conductor. One component of this field E parallel is along x axis represented by a vector arrow and other E perpendicular, is along y axis represented by a vector arrow. Charge inside the conductor moves along x axis so the force acting on it is F parallel, which is equal to q multiplied by E parallel. In part b, a charge is shown inside the conductor and electric field is represented by a vector arrow pointing upward starting from the surface of the conductor.
A conductor placed in an electric field will be polarized. import-auto-id2453144 shows the result of placing a neutral conductor in an originally uniform electric field. The field becomes stronger near the conductor but entirely disappears inside it.
View original figure (external; image not reproduced in this text edition)
Original figure description: A spherical conductor is placed in the external electric field. The field lines are shown running from left to right. The field lines enter and leave the conductor at right angles. Negative charges accumulate on the left surface of the conductor and positive charges accumulate on the right surface of the conductor.
The properties of a conductor are consistent with the situations already discussed and can be used to analyze any conductor in electrostatic equilibrium. This can lead to some interesting new insights, such as described below.
How can a very uniform electric field be created? Consider a system of two metal plates with opposite charges on them, as shown in import-auto-id2594161. The properties of conductors in electrostatic equilibrium indicate that the electric field between the plates will be uniform in strength and direction. Except near the edges, the excess charges distribute themselves uniformly, producing field lines that are uniformly spaced (hence uniform in strength) and perpendicular to the surfaces (hence uniform in direction, since the plates are flat). The edge effects are less important when the plates are close together.
View original figure (external; image not reproduced in this text edition)
Original figure description: Two charged metal plates are shown. The lower plate has negative charge and the upper plate has positive charge. The electric field lines start from positive plate and enter the negative plate represented by arrows.
Earth’s Electric Field
A near uniform electric field of approximately 150 N/C, directed downward, surrounds Earth, with the magnitude increasing slightly as we get closer to the surface. What causes the electric field? At around 100 km above the surface of Earth we have a layer of charged particles, called the ionosphere. The ionosphere is responsible for a range of phenomena including the electric field surrounding Earth. In fair weather the ionosphere is positive and the Earth largely negative, maintaining the electric field (import-auto-id3162895(a)).
In storm conditions clouds form and localized electric fields can be larger and reversed in direction (import-auto-id3162895(b)). The exact charge distributions depend on the local conditions, and variations of import-auto-id3162895(b) are possible.
If the electric field is sufficiently large, the insulating properties of the surrounding material break down and it becomes conducting. For air this occurs at around N/C. Air ionizes ions and electrons recombine, and we get discharge in the form of lightning sparks and corona discharge.
View original figure (external; image not reproduced in this text edition)
Original figure description: In part a, a child is flying a kite with two men in an open field on a bright sunny day. In part b, lightning appears over a body of water in stormy weather.
Electric Fields on Uneven Surfaces
So far we have considered excess charges on a smooth, symmetrical conductor surface. What happens if a conductor has sharp corners or is pointed? Excess charges on a nonuniform conductor become concentrated at the sharpest points. Additionally, excess charge may move on or off the conductor at the sharpest points.
To see how and why this happens, consider the charged conductor in import-auto-id2398984. The electrostatic repulsion of like charges is most effective in moving them apart on the flattest surface, and so they become least concentrated there. This is because the forces between identical pairs of charges at either end of the conductor are identical, but the components of the forces parallel to the surfaces are different. The component parallel to the surface is greatest on the flattest surface and, hence, more effective in moving the charge.
The same effect is produced on a conductor by an externally applied electric field, as seen in import-auto-id2398984 (c). Since the field lines must be perpendicular to the surface, more of them are concentrated on the most curved parts.
View original figure (external; image not reproduced in this text edition)
Original figure description: In part a, a conductor is shown with the unsymmetrical shape. The identical pair of charges at opposite ends on the conductor have similar components of forces represented by arrows. In part b, the unsymmetrical object has positive charge on its surface. The electric field lines are shown emerging perpendicular from the surface of the conductor represented by vector arrow. In part c, the field lines in and around the conductor running from left to right is shown. The left surface of the conductor has negative charge and the right surface has positive charge. The field lines enter and leave the conductor at right angles.
Applications of Conductors
On a very sharply curved surface, such as shown in import-auto-id2677542, the charges are so concentrated at the point that the resulting electric field can be great enough to remove them from the surface. This can be useful.
Lightning rods work best when they are most pointed. The large charges created in storm clouds induce an opposite charge on a building that can result in a lightning bolt hitting the building. The induced charge is bled away continually by a lightning rod, preventing the more dramatic lightning strike.
Of course, we sometimes wish to prevent the transfer of charge rather than to facilitate it. In that case, the conductor should be very smooth and have as large a radius of curvature as possible. (See import-auto-id1993313.) Smooth surfaces are used on high-voltage transmission lines, for example, to avoid leakage of charge into the air.
Another device that makes use of some of these principles is a Faraday cage. This is a metal shield that encloses a volume. All electrical charges will reside on the outside surface of this shield, and there will be no electrical field inside. A Faraday cage is used to prohibit stray electrical fields in the environment from interfering with sensitive measurements, such as the electrical signals inside a nerve cell.
During electrical storms if you are driving a car, it is best to stay inside the car as its metal body acts as a Faraday cage with zero electrical field inside. If in the vicinity of a lightning strike, its effect is felt on the outside of the car and the inside is unaffected, provided you remain totally inside. This is also true if an active (“hot”) electrical wire was broken (in a storm or an accident) and fell on your car.
View original figure (external; image not reproduced in this text edition)
Original figure description: A cone shaped positively charged conductor is shown where most of the positive charges are accumulated at the tip. The field lines represented by arrows emerge at right angles from the surface of the conductor in outward direction. The density of field lines is greater at the tip of the cone than at other surfaces.
View original figure (external; image not reproduced in this text edition)
Original figure description: In part a, a lightning rod is shown on the roof of a house. In part b, a person is touching the metal sphere of the Van De Graaff and his hair is standing up.
Test Prep for AP Courses
View original figure (external; image not reproduced in this text edition) Original figure description: A gold sphere with eight equally spaced black +'s around the outside of the sphere point to eight blue arrows pointing outward. Four of the arrows point directly up, right, down, and left of the sphere and four arrows are equally spaced between these other four arrows at 45 degree angles. The arrow between the left and top arrow is labeled A. The arrow between the top and right arrow is labeled B. The arrow between the right and down arrow is labeled C.
An electric field due to a positively charged spherical conductor is shown above. Where will the electric field be weakest?
- Point A
- Point B
- Point C
- Same at all points
(c)
View original figure (external; image not reproduced in this text edition) Original figure description: There is a gray long thin rectangle at the top of the figure with black pluses. The same size gray long thin rectangle is at the bottom of the figure with minuses below the positives. There are blue lines with an arrow in the middle connecting each + to each -. The two arrows on the left start at the same first + are curved toward the left and hit the first bottom -. The two lines on the right are curved toward the right and connect the last + and -. The six center arrows are vertical. Between line three and four near the + rectangle is an A. A B is between lines four and five near the – rectangle. C is halfway between the + and – rectangle between lines six and seven.
The electric field created by two parallel metal plates is shown above. Where will the electric field be strongest?
- Point A
- Point B
- Point C
- Same at all points
Suppose that the electric field experienced due to a positively charged small spherical conductor at a certain distance is E. What will be the percentage change in electric field experienced at thrice the distance if the charge on the conductor is doubled?
decrease by 77.78%.
View original figure (external; image not reproduced in this text edition) Original figure description: The diagram shows an eye, microscope and then a gray bar with five +'s at the top, 5 arrows pointing directly down to 5 –‘s in a gray bar. In the center of the bars between the + and – bars is a gold drop.
The classic Millikan oil drop experiment setup is shown above. In this experiment oil drops are suspended in a vertical electric field against the gravitational force to measure their charge. If the mass of a negatively charged drop suspended in an electric field of 1.18×10−4 N/C strength is 3.85×10−21 g, find the number of excess electrons in the drop.
Section Summary
- A conductor allows free charges to move about within it.
- The electrical forces around a conductor will cause free charges to move around inside the conductor until static equilibrium is reached.
- Any excess charge will collect along the surface of a conductor.
- Conductors with sharp corners or points will collect more charge at those points.
- A lightning rod is a conductor with sharply pointed ends that collect excess charge on the building caused by an electrical storm and allow it to dissipate back into the air.
- Electrical storms result when the electrical field of Earth’s surface in certain locations becomes more strongly charged, due to changes in the insulating effect of the air.
- A Faraday cage acts like a shield around an object, preventing electric charge from penetrating inside.
Conceptual Questions
Is the object in fs-id1586840 a conductor or an insulator? Justify your answer.
View original figure (external; image not reproduced in this text edition)
Original figure description: External field lines entering the object from one end and emerging from another are shown by lines.
If the electric field lines in the figure above were perpendicular to the object, would it necessarily be a conductor? Explain.
The discussion of the electric field between two parallel conducting plates, in this module states that edge effects are less important if the plates are close together. What does close mean? That is, is the actual plate separation crucial, or is the ratio of plate separation to plate area crucial?
Would the self-created electric field at the end of a pointed conductor, such as a lightning rod, remove positive or negative charge from the conductor? Would the same sign charge be removed from a neutral pointed conductor by the application of a similar externally created electric field? (The answers to both questions have implications for charge transfer utilizing points.)
Why is a golfer with a metal club over her shoulder vulnerable to lightning in an open fairway? Would she be any safer under a tree?
Can the belt of a Van de Graaff accelerator be a conductor? Explain.
Are you relatively safe from lightning inside an automobile? Give two reasons.
Discuss pros and cons of a lightning rod being grounded versus simply being attached to a building.
Using the symmetry of the arrangement, show that the net Coulomb force on the charge at the center of the square below (import-auto-id3009601) is zero if the charges on the four corners are exactly equal.
View original figure (external; image not reproduced in this text edition)
Original figure description: Four point charges, one is q a, second is q b, third is q c, and fourth is q d, lie on the corners of a square. q is located at its center.
(a) Using the symmetry of the arrangement, show that the electric field at the center of the square in import-auto-id3009601 is zero if the charges on the four corners are exactly equal. (b) Show that this is also true for any combination of charges in which and
(a) What is the direction of the total Coulomb force on in import-auto-id3009601 if is negative, and both are negative, and and both are positive? (b) What is the direction of the electric field at the center of the square in this situation?
Considering import-auto-id3009601, suppose that and . First show that is in static equilibrium. (You may neglect the gravitational force.) Then discuss whether the equilibrium is stable or unstable, noting that this may depend on the signs of the charges and the direction of displacement of from the center of the square.
If in import-auto-id3009601, under what conditions will there be no net Coulomb force on ?
In regions of low humidity, one develops a special “grip” when opening car doors, or touching metal door knobs. This involves placing as much of the hand on the device as possible, not just the ends of one’s fingers. Discuss the induced charge and explain why this is done.
Tollbooth stations on roadways and bridges usually have a piece of wire stuck in the pavement before them that will touch a car as it approaches. Why is this done?
Suppose a person carries an excess charge. To maintain their charged status can they be standing on ground wearing just any pair of shoes? How would you discharge them? What are the consequences if they simply walk away?
Problems & Exercises
Sketch the electric field lines in the vicinity of the conductor in fs-id2000560 given the field was originally uniform and parallel to the object’s long axis. Is the resulting field small near the long side of the object?
View original figure (external; image not reproduced in this text edition)
Original figure description: A oblong-shaped conductor.
Sketch the electric field lines in the vicinity of the conductor in fs-id2000561 given the field was originally uniform and parallel to the object’s long axis. Is the resulting field small near the long side of the object?
View original figure (external; image not reproduced in this text edition)
Original figure description: A oblong-shaped conductor.
Sketch the electric field between the two conducting plates shown in fs-id765824, given the top plate is positive and an equal amount of negative charge is on the bottom plate. Be certain to indicate the distribution of charge on the plates.
View original figure (external; image not reproduced in this text edition)
Original figure description: Two plates are shown; one is in horizontal direction and other is above the first plate with some inclination.
Sketch the electric field lines in the vicinity of the charged insulator in import-auto-id1409558 noting its nonuniform charge distribution.
View original figure (external; image not reproduced in this text edition)
Original figure description: A positively charged rod with a concentration of positive charges near the top and a few in the middle.
What is the force on the charge located at in fs-id1996672(a) given that ?
View original figure (external; image not reproduced in this text edition)
Original figure description: Three point charges are shown on the scaling line. First charge plus q is at three point zero, second charge minus two q is at eight point zero, and third charge plus q is eleven point zero centimeters along the x axis. Four charges are placed on a scaling line. First is minus two q at one point zero, second is plus q at five point zero, third is plus three q is at eight point zero, and fourth is minus q placed at fourteen point zero centimeter along the x axis.
(a) Find the total electric field at in fs-id1996672(b) given that . (b)Find the total electric field at in fs-id1996672(b) given that . (c) If the charges are allowed to move and eventually be brought to rest by friction, what will the final charge configuration be? (That is, will there be a single charge, double charge, etc., and what will its value(s) be?)
(a)
(b) one charge of
(a) Find the electric field at in fs-id1996672(a), given that . (b) At what position between 3.00 and 8.00 cm is the total electric field the same as that for alone? (c) Can the electric field be zero anywhere between 0.00 and 8.00 cm? (d) At very large positive or negative values of x, the electric field approaches zero in both (a) and (b). In which does it most rapidly approach zero and why? (e) At what position to the right of 11.0 cm is the total electric field zero, other than at infinity? (Hint: A graphing calculator can yield considerable insight in this problem.)
(a) Find the total Coulomb force on a charge of 2.00 nC located at in fs-id1996672 (b), given that . (b) Find the x-position at which the electric field is zero in fs-id1996672 (b).
(a) 0.252 N to the left
(b)
Using the symmetry of the arrangement, determine the direction of the force on in the figure below, given that and . (b) Calculate the magnitude of the force on the charge , given that the square is 10.0 cm on a side and .
View original figure (external; image not reproduced in this text edition)
Original figure description: Four point charges, one is q a, second is q b, third is q c, and fourth is q d, lie on the corners of a square. q is located at its center.
(a) Using the symmetry of the arrangement, determine the direction of the electric field at the center of the square in import-auto-id2617305, given that and . (b) Calculate the magnitude of the electric field at the location of , given that the square is 5.00 cm on a side.
(a)The electric field at the center of the square will be straight up, since and are positive and and are negative and all have the same magnitude.
(b)
Find the electric field at the location of in import-auto-id2617305 given that , , and the square is 20.0 cm on a side.
Find the total Coulomb force on the charge in import-auto-id2617305, given that , , , , and . The square is 50.0 cm on a side.
in the direction
(a) Find the electric field at the location of in import-auto-id1427585, given that and . (b) What is the force on , given that ?
View original figure (external; image not reproduced in this text edition)
Original figure description: Three point charges located at the corners of an equilateral triangle.
(a) Find the electric field at the center of the triangular configuration of charges in import-auto-id1427585, given that , , and . (b) Is there any combination of charges, other than , that will produce a zero strength electric field at the center of the triangular configuration?
(a) , below the horizontal.
(b) No
Glossary
- conductor
- an object with properties that allow charges to move about freely within it
- free charge
- an electrical charge (either positive or negative) which can move about separately from its base molecule
- electrostatic equilibrium
- an electrostatically balanced state in which all free electrical charges have stopped moving about
- polarized
- a state in which the positive and negative charges within an object have collected in separate locations
- ionosphere
- a layer of charged particles located around 100 km above the surface of Earth, which is responsible for a range of phenomena including the electric field surrounding Earth
- Faraday cage
- a metal shield which prevents electric charge from penetrating its surface